The interest towards a study of strong interaction in the Color Glass Condensate (CGC) setup has been directed to how the configurational entropy (CE) approach can indicate directions for experiments and various methods in QCD [1]}, [2]}, [3]}, [4]}, [5]}.
Answering this question requires knowledge of the information of the total inelastic cross section that could lead to collective nuclear excitations from the point of view of the nuclear configurational entropy and its impact on the fundamental reaction mechanisms
[6]}, [7]}, [8]}.
Analytical and numerical studies have been already devoted to the deep investigation of such techniques concerning various aspects of interaction, including the production of mesons (scalar, vector and tensorial) resonances [9]}, [10]}, [11]}, [12]}, [13]}, [14]}, glueballs [15]}, [16]}, charmonium and bottomonium [17]}, the quark-gluon plasma [18]}, baryonic fields [19]}, and also using the AdS/QCD model approach [20]}.
The configurational-entropic origin of the above mentioned studies can be found in Refs. [21]}, [22]}, [23]}, [24]}, [25]}, [26]}, [27]}.
Extreme points of the CE driving dominant states of physical systems have been also studied and analyzed in Refs. [28]}, [29]}, [30]}, [31]}, [32]}, [33]}, [34]}, [35]}, [36]}, [37]}, also for AdS black holes and their quantum portrait as Bose-Einstein graviton condensates, emulating magnetic structures [38]}.
These critical points manifest the stability and the
predominance of the system states, which also give the vision about the mechanism of interaction for different nuclear systems using, for instance, the CGC for parton saturation effects [5]}, [40]}, [20]}, [6]}, [43]}, [44]}.
Such points have been successfully investigated for the calculation of the inelastic hadron cross sections. The probability of production of different reaction channels can be suggested as spatially localized configurations at high energy regimes [5]}, [6]}, [43]}, [44]}.
